Convolution Theorem (Laplace)
States that the Laplace transform of a convolution of two functions is the product of their individual transforms.
This public page keeps the free explanation visible and leaves premium worked solving, advanced walkthroughs, and saved study tools inside the app.
Core idea
Overview
This theorem provides a powerful method for finding inverse Laplace transforms of products of functions by using the convolution integral.
When to use: Essential for solving non-homogeneous differential equations and analyzing linear time-invariant (LTI) systems.
Why it matters: It converts the complex operation of convolution in the time domain into simple algebraic multiplication in the frequency (s) domain.
Symbols
Variables
F(s)G(s) = L{f * g}, F(s) = F(s), G(s) = G(s)
Walkthrough
Derivation
Derivation/Understanding of Convolution Theorem (Laplace)
This derivation demonstrates that the Laplace transform of the convolution of two functions is equivalent to the product of their individual Laplace transforms.
- The functions f(t) and g(t) are piecewise continuous on [0, ∞) and of exponential order.
- The Laplace transforms F(s) = ℬ{f(t)} and G(s) = ℬ{g(t)} exist.
- The order of integration can be interchanged (Fubini's Theorem applies).
Start with the definition of the Laplace transform of a convolution:
We begin by applying the definition of the Laplace transform to the convolution of two functions, f(t) and g(t), which is itself an integral.
Change the order of integration:
The region of integration is 0 ≤ τ ≤ t < ∞. By changing the order of integration, we rewrite the limits to integrate with respect to t first, then τ.
Perform a substitution in the inner integral:
Let u = t - τ, so t = u + τ and dt = du. This substitution transforms the inner integral into a form that resembles a Laplace transform.
Recognize the Laplace transforms:
The inner integral is the definition of G(s) = ℬ{g(t)}. Factoring G(s) out leaves the definition of F(s) = ℬ{f(t)}, thus proving the theorem.
Result
Source: Kreyszig, E. (2011). Advanced Engineering Mathematics (10th ed.). John Wiley & Sons.
Free formulas
Rearrangements
Solve for F(s)G(s)
Make F(s)G(s) the subject
Start from the Convolution Theorem (Laplace). The expression F(s)G(s) is already isolated, so the task is to identify it as the subject and present it in the target notation.
Difficulty: 1/5
The static page shows the finished rearrangements. The app keeps the full worked algebra walkthrough.
Visual intuition
Graph
The graph typically displays the time-domain representation of two functions and their resulting convolution, often showing smooth, decaying, or oscillatory curves. These curves illustrate the 'memory' effect of a system, where the output at time t is a weighted integral of all past inputs. The interaction between the functions demonstrates how the convolution operation smooths out signals and transforms the system's response into a combined waveform.
Graph type: exponential
Why it behaves this way
Intuition
This theorem provides a powerful 'domain transformation' perspective, where a complex operation like convolution in the time domain is simplified into a straightforward algebraic multiplication in the frequency domain
Free study cues
Insight
Canonical usage
Ensures dimensional consistency between the Laplace transform of a convolution and the product of individual Laplace transforms, where the units of the Laplace variable 's' are inverse time.
Common confusion
Misinterpreting the units of the Laplace variable 's' as dimensionless, or incorrectly handling the units introduced by the integration in the definitions of the Laplace transform and convolution.
Unit systems
One free problem
Practice Problem
Given the individual transforms F(s) = 4 and G(s) = 8, calculate the Laplace transform of the convolution (f * g)(t).
Solve for: result
Hint: According to the theorem, the transform of the convolution is simply the product of the individual transforms.
The full worked solution stays in the interactive walkthrough.
Where it shows up
Real-World Context
In signal processing, the output of a system is the convolution of its input signal and its impulse response; this theorem allows us to find the output using multiplication in the s-domain.
Study smarter
Tips
- The convolution f * g is defined as the integral from 0 to t of f(τ)g(t-τ) dτ.
- Remember that convolution is commutative, meaning f * g = g * f.
Avoid these traps
Common Mistakes
- Confusing convolution f*g with the pointwise product f(t)g(t).
- Forgetting that the theorem only applies if the transforms F(s) and G(s) exist for the same region of convergence.
Common questions
Frequently Asked Questions
This derivation demonstrates that the Laplace transform of the convolution of two functions is equivalent to the product of their individual Laplace transforms.
Essential for solving non-homogeneous differential equations and analyzing linear time-invariant (LTI) systems.
It converts the complex operation of convolution in the time domain into simple algebraic multiplication in the frequency (s) domain.
Confusing convolution f*g with the pointwise product f(t)g(t). Forgetting that the theorem only applies if the transforms F(s) and G(s) exist for the same region of convergence.
In signal processing, the output of a system is the convolution of its input signal and its impulse response; this theorem allows us to find the output using multiplication in the s-domain.
The convolution f * g is defined as the integral from 0 to t of f(τ)g(t-τ) dτ. Remember that convolution is commutative, meaning f * g = g * f.
References
Sources
- Advanced Engineering Mathematics
- Wikipedia: Laplace transform
- Differential Equations with Boundary-Value Problems by Dennis G. Zill
- Dennis G. Zill, Warren S. Wright. Differential Equations with Boundary-Value Problems.
- Erwin Kreyszig. Advanced Engineering Mathematics.
- Wikipedia: Convolution theorem
- Kreyszig, Advanced Engineering Mathematics
- Boyce, DiPrima, and Meade, Elementary Differential Equations and Boundary Value Problems